TFPT scientific source excerpt Original repository path: experiments/theory-contracts/seam-partner-original-action-20261015/PROOF.txt Original file SHA-256: ff7c8dff8939e8380509bff5a34145f935407344a07bda1d65b7b25489a2677c Inclusive original lines: 13-63 Line numbers below refer to the original source. This bounded excerpt is source evidence; it is not a new proof/checker run. Conversation metadata and personal execution details are omitted where indicated. 000013 | 1. ORIGINAL DATA AND THE THREE DIFFERENT OBJECTS 000014 | 000015 | P1 at tfpt_1_architecture_e8.tex:167-188 stipulates an oriented primitive 000016 | reflection-positive seam kernel, unit winding and c3=1/(8pi). P2 stipulates 000017 | five carrier slots with the 3+2 split. Its representation consequences include 000018 | E=C^5=E3 direct-sum E2 and S+=Lambda_even E, with the given hypercharges. 000019 | The original carrier source :573-668 explicitly identifies Lambda^0 E with 000020 | the internal nu^c label. It is NOT the physical vacuum of an affine field net. 000021 | 000022 | Write epsilon_i for exterior multiplication by u_i and iota_i for contraction. 000023 | The quadratic Clifford representation of so(10) has the root operator 000024 | 000025 | A=E_(e1+e4)=epsilon_1 epsilon_4, 000026 | A 1=u_1 wedge u_4. 000027 | 000028 | This fixes an actual nonzero operator and its carrier action, with the stated 000029 | root-vector convention. It is part of the original quadratic-transport algebra 000030 | at architecture :1569-1584; no new interaction has been selected. 000031 | 000032 | Keep these types separate: 000033 | (a) A is a Lie-algebra operator in the adjoint 45; 000034 | (b) A1 is a vector in the half-spinor 16, with weight w_empty+e1+e4; 000035 | (c) |e1+e4>=J_(e1+e4),-1 Omega is an affine root-current state of weight 1. 000036 | The known lattice map M r0=e1+e4 relates root coordinates. It does not identify 000037 | (b) with (c), or the exterior unit 1 with the physical vacuum Omega. 000038 | An infinite affine module is not identified with a finite 16 by this calculation. 000039 | 000040 | 2. WHICH CHARGE IS NEUTRAL? 000041 | 000042 | On the carrier let N_i=epsilon_i iota_i. Original P2 hypercharge is 000043 | 000044 | Y=-(N1+N2+N3)/3+(N4+N5)/2. 000045 | 000046 | The CAR identity gives [N_i,A]=(delta_i1+delta_i4) A. Therefore 000047 | 000048 | [Y,A]=A/6. 000049 | 000050 | The six A_(ia)=epsilon_i epsilon_a, i=1,2,3 and a=4,5, transform as 000051 | (3,2)_(1/6). With T3=(N4-N5)/2, the a=4 and a=5 electric charge shifts are 000052 | 2/3 and -1/3. Changing the weak basis interchanges these labels; neither is zero. 000053 | These are charge changes of the root operator and charges of the carrier vector 000054 | A1 relative to the exterior unit. No physical gauge-boson/fermion equivalence is 000055 | inferred from their common representation label. 000056 | 000057 | The previous fold has a different charge: Q'=2(H3+H6). Its carrier action has 000058 | Q_E=2 diag(0,0,1,0,0), and [dGamma(Q_E),A]=0. This correctly reproduces the 000059 | previous statement that r0 is source-charge neutral. On the six root directions 000060 | the Q' charges are (0,0,0,0,2,2). Thus Q' is not hypercharge and is not central 000061 | under the full color action. This distinction does not invalidate the original 000062 | zero-source-charge calculation; it prevents importing a stronger neutrality. 000063 | FOLD-AUDIT.md:168-230 explicitly conditions this dictionary on the E8 extension.